Pulse pickers - request a quote
The pulse picker consists of the pockels cell, high voltage driver, synchronization and delay generator. It is suitable for single pulse selection from train of femtosecond or picosecond pulses. Also the device is used for pulse slicing in order to increase contrast.
External high-frequency or optical reference High-voltage pulse with adjustable delay High-voltage pulse with adjustable amplitude Two additional sync channels High contrast Low jitter Applications |
When sending us your
request for quotation please indicate the following parameters:
Define the wavelength range that you need the system to operate in. The
wavelength defines the voltage that you need for your application. See the FAQ
section for further explanation on this subject or just send us the desired
wavelength and we will offer the right voltage and ARC.
Check if you need the default 10 ns HV pulse duration (gate open state). E.g. 10
ns duration suits femtosecond pulse train around 80 MHz or 1-5 kHz Ti:Sapphire
amplifier control. Other custom durations and variable modification are
available.
Let us know if you require a 2-channel system or a second Pockels cell.
Pismo pulse picker The Pismo pulse picker systems is as a pulse gating system that lets single pulses or group of subsequent pulses from a femtosecond or picosecond pulse train pass through the system, and stops other radiation. The system is perfectly suitable for most commercial femtosecond oscillators and amplifiers. The system can pick either single pulses, shoot bursts (patterns of single pulses) or pick group of subsequent pulses (wider square-shaped HV pulse modification). HV pulse duration (i.e. gate open time) is 10 ns in the default Pismo 8/1 model, but can be customized from 3 to 1250 ns upon request or made variable. The frequency of the picked pulses starts with single shot to 1 kHz for the basic model, and goes up to 100 kHz for the most advanced one. The Pockels cell is supplied with a control unit that is capable of synching to the optical pulse train via a built-in photodetector unit, while electric trigger signal is also accepted. Two additional delay channels are available for synching of other equipment to the pulse picker operation. Moreover, USB connectivity and LabView-compatible drivers save a great deal of your time on storing and recalling presets, and setting up some automated experimental setups. One control unit is capable of driving of up to 3 Pockels cells, and this comes handy in complex setups or contrast-improving schemes. The system can also be modified to supply two HV pulses to one Pockels cell unit, making it a 2-channel pulse picker system. This may be essential for injection/ejection purposes when building a regenerative or multipass amplifier system. |
Pismo Pulse Pickers brochure - Pismo 8-1-1 manual
Output voltage, kV Repetition rate, kHz Rise time, ns Pulse duration, ns Jitter, ns Input sync signal Sync repetition rate, MHz Adjustable delay, ms |
Pismo 8/1: 4-8; Pismo 12/1: 6-12 1/10/25/50 < 1-10* < 2 -100* < 0.2 optical or TTL 10-150 0 - 4 |
* - please specify with order
Models Pismo 8/2 and Pismo 12/2 incorporate one Pockels cell and produce two
high voltage pulses.
Customer requested high voltage generators up to 50kV are also available.
Pulse shapes from Pismo pulse picker
Del Mar Photonics produce pulse picker systems
with repetition rate up to 100 kHz.
We can offer you our standard devices for picking single pulse from femtosecond
pulse train with following specification:
7 |
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7.1 |
Pismo 8/1. One-channel, 8kV/1Hz-1kHz pulse picker with synchronization electronics |
7.2 |
Pismo 8/10. One-channel, 8kV/500Hz-10kHz pulse picker with synchronization electronics |
7.3 |
Pismo 8/25. One-channel, 8kV/500Hz-25kHz pulse picker with synchronization electronics |
7.4 |
Pismo 8/40. One-channel, 8kV/500Hz-40kHz pulse picker with synchronization electronics |
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Pismo 8/1 (DKDP 10x10x25 mm3) |
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Pismo 88/1 (DKDP 10x10x25 mm3) |
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Pismo 88/1 (BBO 4x4x20 mm3) |
7.5 |
Pismo 12/1. One-channel,12kV/1Hz-1kHz pulse picker with synchronization electronics |
7.6 |
Pismo 12/10. One-channel 12kV/500Hz-10kHz pulse picker with synchronization electronics |
7.7 |
Second channel for pulse picker Pismo 8/1 |
7.8 |
Second channel for pulse picker Pismo 8/10 ; Pismo 12/1 |
7.9 |
Second channel for pulse picker Pismo 8/25 ; Pismo 12/10 |
7.10 |
Pismo 8/1-2. Two-channel, one-cell 8kV/1Hz-1kHz pulse picker with synchronization electronics |
7.11 |
Pismo 55/1. 5kV/1Hz-1kHz /variable 10-1250ns flat top pulse pulse picker with synchronization electronics |
7.12 |
Pismo 88/1. 8kV/1Hz-1kHz /variable 10-1250ns flat top pulse picker with synchronization electronics |
7.13 |
Pismo 8C/1. 8kV/1Hz-1kHz / not variable (constant duration, custom request) flat top pulse pulse picker with synchronization electronics |
7.14 |
Pismo 58P/1. 5kV/1Hz-1kHz /10-1000ns (“zero” square pulse with “prepulse”) pulse picker with synchronization electronics |
7.xx |
Custom Pulse Picker -
please send us your requirements We produce pulse picker system with repetition rate up to 100 kHz (HV pulse have the amplitude ~8kV with duration 10 ns at level 10% of maximum). Contrast ratio - >1000:1, optical transmission of pulse picker system - >87%, clear aperture – 7mm in diameter (other dimension on request), water cooling is required (flow ~3 l/min). |
New models:
1. Pismo OG8-50-1
Pockels cell crystal: DKDP, 6x6x16 mm3, ARC 700-900 nm (clear aperture – 5 mm),
other aperture on request
HV pulse amplitude: up to 8 kV (HV pulse has the amplitude ~8kV with duration 10
ns at level 10% of maximum)
Repetition rate: 1 Hz – 50 kHz
RF source: 30-120 MHz
RF input: optical (internal fiber coupled photodetector with 3m length plastic
fiber)
System transmission: >85%
Contrast ratio: >1:1000
Cooling requirements: water flow ~3 l/min
2. Pismo OG8-100-1
Pockels cell crystal: BBO, 4x4x20 mm3, ARC 700-900 nm (clear aperture – 3.5 mm),
other aperture on request
HV pulse amplitude: up to 8 kV (HV pulse has the amplitude ~8kV with duration 10
ns at level 10% of maximum)
Repetition rate: 1 Hz – 100 kHz
RF source: 30-120 MHz
RF input: optical (internal fiber coupled photodetector with 3m length plastic
fiber)
System transmission: >85%
Contrast ratio: >1:1000
Cooling requirements: water flow ~3 l/min
Pismo Pulse Pickers brochure - Pismo 8-1-1 manual - Del Mar Photonics
Components of a standard pulse picker: 1) Pockels cell 2) Control and supply unit 3) Glan prism 4) Glan prism mount 5) Mirror mount 6) Mirror 7) Quarter-wave plate 8) Fiber 9) Fiber holder 10) AC power cord 11) Connection cable 12) Tube (6 m) |
Del Mar Photonics team member Sergey Tenyakov explains to
Francisco Bezanilla from the
Department
of Biochemistry and Molecular Biology the University of Chicago capabilities of
Pismo pulse picker.
Del Mar Photonics Pismo pulse picker Control and supply unit (oscilloscope is not included).
Pismo pulse picker The Pismo pulse picker systems is as a pulse gating system that lets single pulses or group of subsequent pulses from a femtosecond or picosecond pulse train pass through the system, and stops other radiation. The system is perfectly suitable for most commercial femtosecond oscillators and amplifiers. The system can pick either single pulses, shoot bursts (patterns of single pulses) or pick group of subsequent pulses (wider square-shaped HV pulse modification). HV pulse duration (i.e. gate open time) is 10 ns in the default Pismo 8/1 model, but can be customized from 3 to 1250 ns upon request or made variable. The frequency of the picked pulses starts with single shot to 1 kHz for the basic model, and goes up to 100 kHz for the most advanced one. The Pockels cell is supplied with a control unit that is capable of synching to the optical pulse train via a built-in photodetector unit, while electric trigger signal is also accepted. Two additional delay channels are available for synching of other equipment to the pulse picker operation. Moreover, USB connectivity and LabView-compatible drivers save a great deal of your time on storing and recalling presets, and setting up some automated experimental setups. One control unit is capable of driving of up to 3 Pockels cells, and this comes handy in complex setups or contrast-improving schemes. The system can also be modified to supply two HV pulses to one Pockels cell unit, making it a 2-channel pulse picker system. This may be essential for injection/ejection purposes when building a regenerative or multipass amplifier system. |
Pismo Pulse Pickers brochure - Pismo 8-1-1 manual - Del Mar Photonics
Pismo
10/1-8/1-RTP complete pulse picker system with two Pockels cells
Pulse picker Pismo for Coherent Mira900F 80MHz femtosecond laser
Pismo pulse picker for 1500-1600nm range
Pismo Pulse Pickers: Electro-Optical
Ultrafast Shutters - pdf brochure -
typ.specs -
Pismo pulse picker
for laser wavelength: 1025~1045 nm
Femtosecond Pulse Pickers Pismo Questions and
Answers - 100kHz -
Pismo OG10B/100-1/DKDP 100kHz quote -
Pismo OG10B/100-1/BBO -
Pismo 8-1 Manual -
Pismo 8-10 -
Pismo 8-25 Manual -
QA1
- QA2
- QA3 -
QA4 -
QA5 -
Pockels Cell -
selection of pulses from a ~
100 MHz, 20 fs Ti:Sapphire laser -
pulse selection for polarization
flip - Pulse
peaker for Chameleon Ultra I from Coherent
Pulse picker for Tsunami laser
Pulse
Picker Pismo for Ti:Sapphire laser MIRA Optima 900-D (Femto,Pico) 76 MHz, 800 nm
from Coherent -
Pulse picker for polarization control
Pockels cell based on Rubidium
Titanyle Phosphate – RbTiOPO4 crystal
Ultrafast Shutter
Product news and updates - Training Workshops
- Featured Customer - Other News
Trestles LH Ti:Sapphire
laser Trestles LH is a new series of high quality femtosecond Ti:Sapphire lasers for applications in scientific research, biological imaging, life sciences and precision material processing. Trestles LH includes integrated sealed, turn-key, cost-effective, diode-pumped solid-state (DPSS). Trestles LH lasers offer the most attractive pricing on the market combined with excellent performance and reliability. DPSS LH is a state-of-the-art laser designed for today’s applications. It combines superb performance and tremendous value for today’s market and has numerous advantages over all other DPSS lasers suitable for Ti:Sapphire pumping. Trestles LH can be customized to fit customer requirements and budget. Reserve a
spot in our Femtosecond lasers training
workshop in San Diego, California. Come to learn how to build a
femtosecond laser from a kit |
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DPSS DMPLH lasers |
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New laser spectrometer
T&D-scan for research that
demands high resolution and high spectral
density in UV-VIS-NIR spectral domains - now available with
new pump option! The T&D-scan includes a CW ultra-wide-tunable narrow-line laser, high-precision wavelength meter, an electronic control unit driven through USB interface as well as a software package. Novel advanced design of the fundamental laser component implements efficient intra-cavity frequency doubling as well as provides a state-of-the-art combined ultra-wide-tunable Ti:Sapphire & Dye laser capable of covering together a super-broad spectral range between 275 and 1100 nm. Wavelength selection components as well as the position of the non-linear crystal are precisely tuned by a closed-loop control system, which incorporates highly accurate wavelength meter. Reserve a
spot in our CW lasers training
workshop in San Diego, California. Come to
learn how to build a
CW
Ti:Sapphire laser from a kit |
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Near IR viewers Ultraviolet viewers are designed to observe radiation emitted by UV sources. |
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AOTF Infrared Spectrometer |
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Open Microchannel Plate Detector
MCP-MA25/2 -
now in stock! |
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Hummingbird EMCCD camera The digital Hummingbird EMCCD camera combines high sensitivity, speed and high resolution. It uses Texas Instruments' 1MegaPixel Frame Transfer Impactron device which provides QE up to 65%. Hummingbird comes with a standard CameraLink output. It is the smallest and most rugged 1MP EMCCD camera in the world. It is ideally suited for any low imaging application such as hyperspectral imaging, X-ray imaging, Astronomy and low light surveillance. It is small, lightweight, low power and is therefore the ideal camera for OEM and integrators. buy online |
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Hatteras-D
femtosecond transient absorption data acquisition system Future nanostructures and biological nanosystems will take advantage not only of the small dimensions of the objects but of the specific way of interaction between nano-objects. The interactions of building blocks within these nanosystems will be studied and optimized on the femtosecond time scale - says Sergey Egorov, President and CEO of Del Mar Photonics, Inc. Thus we put a lot of our efforts and resources into the development of new Ultrafast Dynamics Tools such as our Femtosecond Transient Absorption Measurements system Hatteras. Whether you want to create a new photovoltaic system that will efficiently convert photon energy in charge separation, or build a molecular complex that will dump photon energy into local heat to kill cancer cells, or create a new fluorescent probe for FRET microscopy, understanding of internal dynamics on femtosecond time scale is utterly important and requires advanced measurement techniques. Reserve a
spot in our Ultrafast Dynamics Tools
training workshop in San Diego, California. |
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Beacon Femtosecond Optically Gated Fluorescence Kinetic Measurement System
-
request a quote -
pdf Reserve a
spot in our Ultrafast Dynamics Tools
training workshop in San Diego, California. |
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Terahertz systems, set ups and components New band pass and long pass THz optical filters based on porous silicon and metal mesh technologies. Band pass filters with center wavelengths from 30 THz into GHz range and transmissions up to 80% or better. Standard designs with clear aperture diameters from 12.5 to 37.5 mm. Long pass filters with standard rejection edge wavelengths from 60 THz into GHz range. Maximum transmission up to 80% or better, standard designs at 19.0 and 25.4 mm diameters. Excellent thermal (from cryogenic to 600 K) and mechanical properties THz products: THz Spectrometer kit with Antenna THz transmission setup THz time domain spectrometer Pacifica fs1060pca THz time domain spectrometer Pacifica fs780pca THz detectors: Golay cell and LiTaO3 piroelectric detectors PCA - Photoconductive Antenna as THz photomixer Pacifica THz Time Domain Spectrometer - Trestles Pacifica Holographic Fourier Transform Spectrometer for THz Region Wedge TiSapphire Multipass Amplifier System - THz pulses generation Terahertz Spectroscopic Radar Mobile System for Detection of Concealed Explosives Band pass filters with center wavelengths from 30 THz into GHz range Long pass filters with standard rejection edge wavelengths from 60 THz into GHz range Generation of THz radiation using lithium niobate Terahertz crystals (THz): ZnTe, GaAs, GaP, LiNbO3 - Wedge ZnTe |
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iPCA - interdigital Photoconductive Antenna for terahertz waves Large area broadband antenna with lens array and high emitter conversion efficiency iPCA with LT-GaAs absorber, microlens array for laser excitation wavelengths l £ 850 nm, adjusted hyperhemispherical silicon lens with a high power conversion efficiency of 0.2 mW THz power / W optical power. The iPCA can be used also as large area THz detector. The two types iPCAp and iPCAs have the same active interdigital antenna area but different contact pad directions with respect to the electrical THz field. Interdigital Photoconductive Antenna for terahertz waves generation using femtosecond Ti:Sapphire laser THz books |
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IntraStage lowers the cost
of test data management! Struggling with gigabytes or terabytes of test data? IntraStage easily transforms test data from disparate sources into web-based quality metrics and engineering intelligence you can use.
Contact
us today to discuss your test management requirements and specifications of your
application. |
Training Workshops
Come to San Diego next summer! Attend one of our training workshops in San Diego, California
during summer 2011 Del Mar Photonics has presented training workshops for customers and potential customers in the past 3 years. Our workshops cover scientific basics, technical details and provide generous time for hands-on training. Each workshop is a three-day seminar conducted by professional lecturer from 10am to 4pm. It includes lunch, as well as a training materials. We have also reserved two days for Q&A sessions, one-on-one system integration discussions, social networking, and San Diego sightseeing.
The following training workshops will be offered during this
summer: |
Featured Customer
Trestles LH10-fs/CW laser system at UC Santa Cruz Center of Nanoscale Optofluidics
Del
Mar Photonics offers new
Trestles fs/CW laser system which can be easily
switched from femtosecond mode to CW and back. Having both modes of operation in one system dramatically increase a
number of applications that the laser can be used for, and makes it an ideal
tool for scientific lab involved in multiple research projects. |
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Frequency-stabilized CW single-frequency ring Dye laser DYE-SF-007 pumped by DPSS DMPLH laser installed in the brand new group of Dr. Dajun Wang at the The Chinese University of Hong Kong. DYE-SF-077 features exceptionally narrow generation line width, which amounts to less than 100 kHz. DYE-SF-077 sets new standard for generation line width of commercial lasers. Prior to this model, the narrowest line-width of commercial dye lasers was as broad as 500 kHz - 1 MHz. It is necessary to note that the 100-kHz line-width is achieved in DYE-SF-077 without the use of an acousto-optical modulator, which, as a rule, complicates the design and introduces additional losses. A specially designed ultra-fast PZT is used for efficient suppression of radiation frequency fluctuations in a broad frequency range. DYE-SF-077 will be used in resaerch of Ultracold polar molecules, Bose-Einstein condensate and quantum degenerate Fermi gas and High resolution spectroscopy |
Other News
Optical Society of Southern California meeting at UCSD OSSC 2011-04-27
Nd:YAG laser ordered by the University of Leon, UANL, Mexico
Wedge 50 Multipass Amplifier pumped with a Darwin-527-30-M DPSS Laser
ordered by Hong Kong customer
New
Trestles LH10-fs/CW femtosecond+CW laser ready for delivery to the
University of California Santa Cruz
Trestles femtosecond
Ti:Sapphire laser delivered to North Carolina State
University
Del Mar Photonics sponsor IONS (International OSA Network of Students)
conference IONS-NA-2 in Tucson, Arizona
IONS-NA-2
website
Best talk and best
poster awards at IONS-Moscow 2010 conference sponsored by Del Mar Photonics
Watch Del Mar Photonics
videos!
Del Mar Photonics is now on Twitter!
Del Mar Photonics featured components
Del Mar Photonics continuously expands its components portfolio.
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Solar
Prisms for Concentrating Photovoltaic Systems (CPV) Solar cells made of compound semiconductors such as gallium arsenide are very expensive. Usually very small cells are installed and various means such as mirrors, lenses, prisms, etc..are used to concentrate sunlight on the cells. Concentration photovoltaic technology (CPV) uses the solar radiation with an efficiency of 40%, double that of conventional solar cells Del Mar Photonics design custom Concentrating Photovoltaic Systems (CPV) and supply variety of the optical components for CPV such as solar prisms shown in the picture. |
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Axicon Lens Axicon lens also known as conical lens or rotationally symmetric prism is widely used in different scientific research and application. Axicon can be used to convert a parallel laser beam into a ring, to create a non diffractive Bessel beam or to focus a parallel beam into long focus depth. Del Mar Photonics supplies axicons with cone angles range from 130° to 179.5° for use with virtually any laser radiation. We manufacture and supply axicons made from BK7 glass, fused silica and other materials. download brochure - request a quote |
Rutile (TiO2) coupling
prisms Del Mar Photonics offers optical elements made of high quality synthetically grown Rutile Titanium Dioxide crystals. Rutile’s strong birefringency, wide transmission range and good mechanical properties make it suitable for fabrication of polarizing cubes, prisms and optical isolators. Boules having high optical transmission and homogeneity are grown by proprietary method. Typical boules have 10 - 15 mm in dia. and up to 25 mm length. Optical elements sizes - from 2 x 2 x 1 mm to 12.7 x 12.7 x 12.7 mm. Laser grade polish quality is available for finished elements. So far we the largest elements that we manufactured are 12 x15 x 5 mm, in which optical axis is parallel to 15 mm edge, 5 mm is along beam path, 12 x 15 mm faces polished 20/10 S/D, one wave flatness, parallelism < 3 arc.min. (better specs. available on request). more details - download brochure - request a quote |
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Sapphire components Sapphire Circular Windows - Square & Rectangle - Rods Sapphire & Ruby Rings - Sapphire & Ruby Balls - Sapphire & Ruby Nozzles Sapphire Lenses - Ball & Seat - Special Products - Sapphire Vee & Cup Jewels Sapphire Ceramics - Ceramic Sleeves - Ceramic Holes - Ceramic Rods Sapphire & Ruby Orifices - Sapphire & Ruby Tubes - Sapphire Components Sapphire Half Round Rod - Sapphire Windows - Rods & Tubes - Special Part Sapphire Prism - Sapphire Chisel - Sapphire Square Rod |
Vacuum viewport Del Mar Photonics offer a range of competitively priced UHV viewports , Conflat, ISO or KF including a variety of coatings to enhance performance. Del Mar Photonics viewports are manufactured using advanced techniques for control of special and critical processes, including 100 percent helium leak testing and x-ray measurements for metallization control. Windows Materials include: Fused silica, Quartz , Sapphire , MgF2, BaF2, CaF2, ZnSe, ZnS, Ge, Si, Pyrex. Standard Viewing diameters from .55" to 1.94 ". Coating - a range of custom coatings can applied - which include - Single QWOT - Broad Band AR - V coatings - ITO - DLC (Diamond like coating) more details - request a quote |
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Hydrogen
Thyratrons are used in
such devices as radars with different power levels, high-power pulsed
technical, electrophysical, medical devices and lasers. Sophisticated
design and high quality ceramic-metal envelope determines long lifetime
and very accurate and reliable operation of hydrogen thyratrons under wide range of environmental
conditions. Applications: - radars - pulsed lasers power supplies - medical apparatus - electrophysical instrumentation Triggered Three-Electrode Spark Gap Switches are ceramic-metal sealed off gas discharge trigatron-type devices with a co-axial trigger electrode. These Gas Discharge Tubes contain no mercury and, due to an advanced design, feature high reliability and a long lifetime being operating under wide range of environmental conditions. Applications: - pulsed installation for processing materials - installations with plasma focus - pulse power supplies for lasers and other pulse equipment - medical apparatus such as lithotriptors and defibrillators - processing systems for petroleum wells |
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Trigger Transformers Del Mar Photonics supply trigger transformers for triggered spark gaps and other applications. Contact us to today to discuss your application or requesta quote. Trigger Transformers are used to provide a fast high voltage pulse up to 30kV/µs and more. This high voltage pulse is applied to the trigger electrode to initiate switching action in the three-electrode spark gaps. Either positive or negative pulses can be obtained from all of the transformers.
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We are looking forward to hear from you and help you with your optical and crystal components requirements. Need time to think about it? Drop us a line and we'll send you beautiful Del Mar Photonics mug (or two) so you can have a tea party with your colleagues and discuss your potential needs. |
Del Mar Photonics, Inc.
4119 Twilight Ridge
San Diego, CA 92130
tel: (858) 876-3133
fax: (858) 630-2376
Skype: delmarphotonics
sales@dmphotonics.com